Related Experiment Video
Updated: May 24, 2026

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
Models of radiofrequency coupling for negative ion sources
1INFN-LNL, viale dell'Universita n.2, 35020 Legnaro (PD), Italy. cavenago@lnl.infn.it
The Review of Scientific Instruments
|March 3, 2012
Summary
Radiofrequency heating in inductively coupled plasma (ICP) ion sources is influenced by various factors. This study presents an effective plasma conductivity model and its application in plasma transport and heating simulations for small sources.
Area of Science:
- Plasma Physics
- Ion Source Technology
- Radiofrequency Heating
Background:
- Radiofrequency (RF) heating is crucial for inductively coupled plasma (ICP) ion sources.
- Heating efficiency is affected by operating pressure, Faraday shield, coil geometry, frequency, and magnetic fields.
- A magnetic filter is essential for H(-) ion survival in negative ion sources.
Purpose of the Study:
- To investigate factors influencing RF heating in ICP ion sources.
- To present an effective plasma conductivity model.
- To demonstrate the application of this model in plasma transport and heating simulations.
Main Methods:
- Single particle simulations were used to analyze electron acceleration.
- An effective plasma conductivity model was developed, incorporating static magnetic field effects.
- Multiphysics tools were employed for plasma transport and heating modeling.
Main Results:
- Electron acceleration was observed in the preglow regime for a 15 cm driver chamber radius.
- The effective plasma conductivity depends on electron density, temperature, RF field, and static magnetic field.
- The developed conductivity model was successfully applied to a small ICP source.
Conclusions:
- The study provides insights into optimizing RF heating in ICP ion sources.
- The new plasma conductivity model enhances the accuracy of plasma transport and heating simulations.
- The findings are relevant for the design and operation of ICP ion sources, particularly for negative ion generation.
Related Concept Videos
Double Resonance Techniques: Overview
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
Mass Analyzers: Common Types
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
Generating Electromagnetic Radiations
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in the...
Van de Graaff Generator
Van de Graaff generators (or Van de Graaffs) are devices used to demonstrate high voltage due to static electricity that can also be used for research. Robert Van de Graaff first built one in 1931 (based on original suggestions by Lord Kelvin) for use in nuclear physics research.
Van de Graaff uses both smooth and pointed surfaces, conductors, and insulators to generate large static charges and, hence, large voltages. A substantial excess charge can be deposited on the sphere because it moves...
Van de Graaff uses both smooth and pointed surfaces, conductors, and insulators to generate large static charges and, hence, large voltages. A substantial excess charge can be deposited on the sphere because it moves...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
¹³C NMR: ¹H–¹³C Decoupling
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
